Electro-optical system



March 14, 1939. F. GRAY ELEcT-OP'MCAL SYSTEM Filed March 4, 1936 .2 Sheets-Sheet l /NVE NT g? By @GRA A77' RNEV March 14, 1939. F GRAY 2,150,159

ELECTRO-OPTICAL SYSTEM Filed March 4, 1956 2 Sheets-Sheet 2 /NVENTOR E GRA V av ATZ' RNEV Patented Mar. 14, 193e 2,150,159

UNITED STATES PATENT oFFicE amuse memo-OPTICAL srs'rmu Frank Gray, New York, N. Y., assigner to Bell Telephone Laboratories, Incorporated, New York, N. Y., a corporation of New York Application March 4, 1936, Serial No. 67,059 4 Claims. (Cl. TIS-7.2)

This invention relates to electro-optical sys- Associated with the container are means for aptems and more particularly to a method of and plying radiations of the rst wave-length range means for setting up electric currents representato an object and for directing radiations reflected tive of the various light-tone values of an object, from the object, through the interstices of the 5 as in television scanning. mesh electrode and the photo-emissive layer,

Certain light sensitive electric materials have 'a upon the photo-conducting nlmto control its conlarge response to light of wave-lengths within a ductivity. Also associated with the container are certain range and zero or negligibly small re- `means for producing amoving beam of radiations sponse in another range or ranges. It has been of the second wave-length range and for causing discovered that this phenomenon can be put to it to pass through the interstices of the electrode 1 use in electro-optical systems, as for example, to scan successively the elemental areas of the television transmission systems, so that a lightphoto-emissive coating, which is thereby activatsensitive electric image receiving plate or layer ed to cause the production ef a mcving beam 0f may be associated with a second light-sensitive electrons Which Passes t0 the mesh electrode. t0

electric layer adapted to be scanned by av beam of thereby cause a flow of image current to an ex- 1 light to produce image currents dependent upon ternal circuit. The flow of photo-electrons from the light intensities of the elemental areas ofthe an elemental area of the phcto-emissivc coating image plate, the material of one or both layers is controlled by the Conductivity imparted t0 s110- being chosen with regard to the wave-length cessive elemental areas of the .underlying photorange of sensitivity, and the wave-lengths oi Conducting layer by radiations COI'IesDOnding t0 .1

either the scanning beam lor the image light the lights and shades 0f the Objectbeam, or both, also being chosen so that one or As an alternative, radiations reiiected from the the other of these beams may pass through one Object may be applied te the photo-emissive coatlayer to the other without affecting it, or each ing from a Wave-length range Which Cause it t0 beam may impinge upon both layers while aiectemit electrons but Which d0 not affect, the 00ni ing only one, or each beam may impinge upon duetivity of the photo-conducting lm and an a different layer, thus each beam affecting only image Current may be prOdueed by Scanning the one, photo-conducting lm with a beam. of radiations An object of this invention is to provide methwhich renders its elemental areas conductive in 3() ods of and apparatus for utilizing the phenomturn but Which does D015 cause the photo-emisSiVe 1 enon mentioned above in the production of elec- Coating t0 emit electrons. tric currents under control of light. In anOthel embodiment, the target may ccm- Another object is to provide novel means for prise a metal Plate, a pail 0f PhOtO-eOndllcting producing image currents for use in systems of lms Of materials respectively sensitive to diftelevision and telephotography, ferent wave-length ranges of radiations, and a A further objeot of this invention is to provide transparent conductive layer. Radiations of one scanning apparatus which, while not utilizing the range reeeted fl'Om the Obleet Control the 00nphenomenon mentioned above, provides means duCtiVitY 0f the elemental areas 0I one 0f the for making each lm 0r layer responsive t0 a, lmS in'aCCOldallCe with the light-t0n@ Values 0f 40 different beam of light, the corresponding elemental areas of the object In accordance with one embodiment of the in- While a beam 0f radiations 0f a Second wavevention, chosen for purposes of illustration andv length range Scans in succession the elemental hereinafter described in detail, a gas-tight con- 'areas of the second lm through the transparent tainer encloses a target, comprising a metallic layer and the rst film to successively render plate carrying a photo-conducting lm, i, e., a these elemental areas conducting. The external film formed of material adapted to have itscon- 'circuit is connected to the metal plate and the ductivity increased when supplied with radia.- transparent conductive layer, so that when the tions of one wave-length range, on which is elemental areas of both lms are made conductapplied a very thin nlm or coating of a noning by the radiations projected on'them respecconducting photo-emissive material adapted to tively, an. image current which varies with the emit electrons when exposed to radiations of a tone values of the object passes through this exsecond wave-length range which radiations, howternal circuit.' Y 'ever, do not aect the conductivity of the photo- As an alternative to this embodiment, the conducting nlm, and a ne mesh electrode adjatarget may comprise a transparent plate procent the coatingy of photo-emissive material. vided with a transparent metal coating carrying two superposed lms of photo-conducting material, and a transparent conducting layer, the image controlled radiations being applied to one ilm from a position in front of the target to control the conductivity applied to its respective unit areas, as described above, while the scanning beam of radiations of a different wave-length range is directed through the transparent plate to the other fllm from a position behind the target. 'I'he external circuit is connected between the metal coating and the conducting layer and an image current is supplied to that circuit in a manner similar to. that described above. The target may be applied to the external surface of the end wall of a cathode ray tube, i. e., the wall carrying the iiuorescent screen, and radiations from the'fluorescent spot may be used to effect scanning. Again, the target may comprise two photo-conducting lms of the same material separated by an intervening black, high resistance layer, which prevents the scanning spot from aiiecting the photo-conducting iilm to which the image controlled radiations are applied. As a further' alternative, a single film of photo-conducting material may be used, provided it is just thick enough to prevent the scanning spot and the radiations controlled by the object from affecting it throughout. In either of the two lastmentioned alternatives, radiations of the same type may be used both for illuminating the object and for scanning the target.

Ii.' the photo-conducting layers in any of the above embodiments are 'made of a material having high specific resistance and are made relatively thin compared to the size of the area covered by the scanning light beam, they may be made continuous as the lateral conductivity therethrough be so small as to be negligible. The thin film and the high specific resistance help to produce a large stored charge which is discharged by the scanning beam.

The invention will be more readily understood by referring to the following description, taken in connection with the accompanying drawings forming a part thereof, in which:

Fig. l is a diagrammatic representation of a television system including the invention;

Fig. 2 is an enlarged perspective view oi' the assembly used in the scanning tube oi' Fig. 1;

Fig. 3 is an enlarged perspective view of a type of assembly that may be used as an alternative to that shown in Fig. 2;

Fig. 4 shows a system somewhat similar to that of Fig. 1 embodying a moditled method of scanning;

Fig. 5 is an enlarged perspective view of the assembly used in the scanning tube of Fig. 4;

Fig. 6 shows an image target mounted on the end oi' a cathode ray tube; and

Figs. '7 and 8 are modications o1' Fig. 6.

Referring more particularly to the drawings, Fig. 1 shows a television system which, in general. comprises a television transmitter T connected by a transmission channel L to a television receiver, R.

'Ihe transmitter T includes a scanning tube S.

an optical system ior gathering radiations -of one type, reilected from an object O, and for directing these radiations to a target included in the scanning tube, and means, such 'as the cathode ray tube C, for producing a moving beam of radiations of a second type and, in cooperation with a suitable optical system, for causing this beam to scan the target. Scanning tube S comprises a gas-tight container I of glass or other suitable material enclosing an image target or screen, represented generally as II, and a ne mesh electrode I2 spaced therefrom.

In order to clarify the detailed description of the system of Fig. 1, reference will now be made to Fig. 2, which illustrates an enlarged perspective view of the assembly used in the scanning tube S, with the glass container broken away. As therein shown, the assembly comprises a suitable anode, such as the mesh electrode I2 and a target or screen II comprising in order (starting from the side away from the electrode I2): a metal plate I3 carrying a photo-conducting nlm I4 which in turn carries a coating I5 of photo-emissive material. The conductivity of the photo-conducting ilm I4 increases when supplied with radiations of one wave-length range, which for convenience will be hereinafter designated A-radiations, while the photo-emisslve coating I5 is sensitive to a second wave-length range of radiations, hereinafter designated B- radiations, which do not affect the conductivity of the fllm I4. Y

The ne mesh electrode I2 is adjacent the photo-emissive coating I5 and is connected to the metal plate I3 by an external circuit, including a battery I6 and a resistance I1, the latter being included in the input circuit of an ampliiier I8. The negative terminal of the battery I6 is connected to the metal plate I3 and the batterys positive terminal is connected to the mesh electrode I2 through the resistance I1, whereby this electrode is polarized to operate as an anode with respect to the plate I3.

'Ihe object or iield of view O is supplied with radiations from a suitable source, not shown, and these radiations are reected from the object through an optical system, represented generally by a lens I9, through the interstices of the mesh electrode I2 and through the thin coating I5 onto the photo-conducting lm I4 where an image of the object 0 in A-radiations is formed. The small areas of the lm Il are thereby successively rendered conducting in accordance with the tone values of the corresponding small areas of the image iield 0. A suitable optical lter 20 may be inserted between the object O and the lens I9 in order to pass only the type of radiations desired.

Also associated with the scanning device S is a second optical system represented by a means for generating a moving spot of light, and a lens system, represented generally by a lens 2|, for forming a moving beam of radiations to scan the surface of the photo-emissive coating I5. -The means for generating* the moving spot of light is represented andywill be described below as a cathode ray tube C having a fluorescent screen 22, but any other suitable type of apparatus for producing this' result may be used, as for example, a source of radiations associated with a disc having a series of apertures arranged1 in la spiral.

The cathode beam of the tube C is deflected in two directions at right-angles to each other and at such relative speeds in the two directions that the screen 22 is excited to fluorescence to produce a moving spot of radiations which covers the entire screen in a time interval within the period of persistence of vision, in order to prevent iiicker. Deilection of the beam in one direction is effected by the field between a pair of deflecting plates 23 supplied with current having a sawtocthed wave form', the production of this current rent of line scanning frequency received from the I eing controlled by oscillations of line scanning requency supplied by the oscillator 24 to the eecting-current producing device 25. Deilec- Lon in the other direction is produced by suplying a second pair of deflecting plates 26 With current, also of saw-tooth wave forni, supplied y the deiiecting-current producing device 21, ontrolled by oscillations of image cycle frequency roduced by a sub-harmonic generator 28 suplied with oscillations from the oscillator 24. Any uitable apparatus, such as that 4disclosed in lnited States Patent 1,613,954, January 11, 1927, o Knoop, may be used to produce the deflecting urrents.

The operation of the scanning tube S is as ollows:

A-radiations from a suitable source (not hown) are reflected by the object O and proected through the interstices of the mesh elecrode I2 and the photo-emissive coating I5 upon he photo-conducting film I4. These A-radiaions increase the conductivity of the film I4 but lo not'aiect the layer I5. A beam of radiations rom the moving spot of light produced by the luorescent screen 22 is directed by the lens sysem 2l through the interstices of the mesh elecrode I2 to scan successively the elemental areas rf the photo-emissive coating I5. These radia- `ions are of the second, or B-type, and cause the :oating I to be activated'to cause the ow of a noving beam of photo-electrons to the mesh elecyrode I2; the flow from any elemental area being :ontrolled by the conductivity imparted to the :orresponding elemental area of the photo-conlucting iilm I4 by the radiations reiiected by the )bject O. In lother Words, the resistance of the :ircuit through the tube at any instant is dependent upon the resistance-of the elemental area of ;he photo-conducting lm I4 which corresponds so the elemental area of the photo-emissive coatlng I5 being scanned at that time. The resistance of the elemental areas of the lm I4 1s determined by the intensity of the radiations re- Elected from the object O onto the successive elemental areas of the lm. Thus, an image current varying with the tone values of successive elemental areas of the image O is caused-to flow through the external circuit including a resistance I1, as described above, Where'it is supplied; after amplication by the device I8, to a transmission circuit and over a line L, or a line carrier or radio channel, to a distant receiving station which includes a receiver R.

Receiver R may include an amplifier, in case the image current is directly transmitted, or a demodulator and amplier in case transmission is effected in accordance with line carrier or radio practice. It may also include a cathode ray discharge device 30 comprising a cathode 3l andan anode 32 for producing the cathode beam, two pairs of plates 33 and 34 for respectively effecting deflection of the beam in two directions at right-angles to each other, a fluorescent screen 35, and a pair of control grids 36 and 31 connected by an external circuit 38 to which the image currents received over line L and amplied by the device 39 are supplied by means of a transformer 40. Auxiliary devices 4I, 42 and 43, similar to those described in connection with the transmitter, are also used in the receiving system R. Devices 4I and 42 operate, as disclosed in the Knoop patent, to supply deflecting current of saw-tooth wave form to respective pairs of deecting plates 34 and 33. The apparatus for producing the deecting current is controlled by curfeeders have been designated as L' and L".

oscillator 24 via a transmission line or radio channel, which has not been shown, but its In this manner, the cathode beam of the receiver R, is deected in synchronism and in phase with the deection of the cathode ray beam of the discharge device C used at the transmitter.

The cathode ray discharge device 30 at the receiving station operates in the following manner:

The control electrodes or grids 36 and 31 are closely adjacent each other in a position between the anode 32 and the fluorescent screen 35 and comprise segments of a sphere, the centers of which are close to the centers of the deflecting elds produced by the pairs of plates 33 and 34.

The grid 36 is maintained at substantially thel same potential as the anode 32 and the signal potentials are applied to the grid 31, which may be negatively polarized with respect to the grid 36. The two grids, therefore, serve to denne a very limited zone in which the signal potentials are effective for controlling the cathode beam, and this zone is substantially isolated from the equipotential section established between the anode 32 and the grid 36, within which zone de flection of the beam is effective. Consequently, deflection of the beam is controlled by the fields established between the pairs of plates 33 and 34 Without being influenced by the signal potentials, and the signal potentials operate to control the velocity or number of electrons constituting the beam and hence the intensityof the excitation of the fluorescent screen, which determines the quality of the image produced, Without causing the direction of travel of the electrons to be varied. In other words, the two sets of elements for eiectively controlling the deection and intensity of the beam, each of which tends to interfere with the other and thereby cause loss of focus of the beam and distortion oi the image, are so positioned and electrically controlled as to materially, if not completely, avoid such interference. For a more complete disclosure of the construction and method of operation of the image producing cathode ray device 30 briefly described above, reference may be made to application Serial No. 466,067 of J. B. Johnson, led July 7,

While a receiver of the cathode ray discharge type has been described, it will, of course, be obvious that a glow lamp cooperating with a revolving disc having a spiral of apertures, or any other Well-known receiver may be used with my invention. A satisfactory receiver of the glow lamp type is disclosed in United States Patent 1,728,122, September 10, 1929, to Horton.

'I'he A-radiations may be red or infra-red, 01 in other Words, those radiations having a wavelength greater than about 6500 Angstrom units, while the B-radiations may be blue, violet, or ultra-violet, or in other words, those radiations having a wave-length less than about 4700 Angstrom units. The wave-lengths given above are merely by way of example and this invention is not specifically limited thereto. While in Fig. 1 a system has been described in which the object has applied thereto A-radiations while the scanning beam is of B-radiations, it is to be understood that B-radiations may be used to reilect an image of the object onto the photo-emissive coating I5, whereby it is actuated to cause the emission of electrons, these B-radiations not aiecting the conductivity of the photo-conducting film I4; and the iilm I4 may be scanned with a beam of A-radiations which affects its conductivity but which does not cause electronic emission from the layer I5. The scanning beam in this arrangement renders the elemental areas of the film I4 successively conductive as they are scanned in turn.

The cathode ray tube is well suited for use as a source for supplying a scanning beam of B- radiations as the spot of light given oi by the fluorescent screen is rich in radiations in the blue, violet and ultra-violet portions of the spectrum. If ultra-violet radiations are used for the scanning beam, the lens in the optical system 2I as Well as the material of the enclosure should be of a suitable substance to pass the radiations such as, for example, quartz. Also, -it might be desirable in some cases to include within the optical system represented by 2l a suitable optical lter to lter out all undesired radiations.

The assembly shown in Fig. 2 may comprise a lm I4 of selenium or other suitable material made of discrete particles so that the lateral conductivity is negligibly small. The lm may be in globular form. Selenium is particularly sensitive` to red and infra-red radiations. The very thin, and hence, discontinuous transparent, photoemissive coating I5 may be made of a suitable alkali metal sensitive to blue, violet, or ultraviolet radiations, such as for example, potassium hydride. The lm I4 may comprise a thin, continuous lm which may have its lateral conductivity decreased by cross-hatching the lm with iine lines through to the metal plate I 3, or the surface of the metal plate may be cross-hatched with numerous, deep, and narrow grooves.

The operation described above may be called the resistance method. If the thin lm I4 is of suiiiciently high specic resistance, the device will operate by another method, that is, by the so-called storage method because charges are laid down on one surface of the photo-conducting element which leak oil! during the next image cycle, the` recharging current thus forming a greatly increased image current.- This high speciflc resistance also makes possible the use of a continuous film of photo-conducting material while still restraining the lateral conductivity to a negligible minimum, provided that the thickness of the illm is small compared to the diameter of the scanning spot, that is, for example, onetenth of that diameter. For a more complete description of the "storage method of operation in comparison with the "resistance method, and the relation of lateral to transverse conductivity in thin high resistance films reference may be made to application Serial No. 67.058, illed March 4, 1936, for Frank Gray. 'A suitable photo-conducting material which is of suwfilciently high specific resistance to operate in accordance with the storage method and which is sensitive to red or infra-red radiations is mercuric iodide (Hgh) An enlarged perspective view o1' a modiiied scanning tube is shown in Fig. 3. In this embodiment there is no mesh electrode, the external circuit being connected between the metal plate and a light transmitting conducting layer on the target. The composite target 4`| comprises a metal plate I3 carrying two photo-conducting illms 44 and 45 of different materials and a transparent conducting layer 48. 'Ihe `conductivity of the photo-conducting lm 44 is changed by B- radiations, but is not affected by A-radiations. Inthe case of the photo-conducting lm 45, the reverse is true as its conductivity is changed by VA-radiations, but is unaffected by B-radiations.

parted to small areas of the rst lm by A-radiations, ows through the external circuit. If the second iilm 44 is made very thin and of high specific resistance when dark (that is, when not 4 illuminated with the radiations to which it is sensitive), there is provided between the rst lm 45 and the metal plate I3 a capacity in which image impulses, corresponding to the elemental areas of the image, may be stored and hence a greatly increased image current flow is produced in the external circuit, which circuit is similar to that shown in Fig. 1. If the A-radiations are red or infra-red, the photo-conducting film 45 may be selenium for the resistance method or mercury iodide for the storage method and a photo-conducting film 44, sensitive to B-radiations (blue, violet, or ultra-violet), may consist of thallium bromide or chloride which may be used for either method as the specific resistance of the lm 44 when illuminated does not have tobeashighasthatofthelmasthislm44 is used to .discharge the stored charge rather than to store it up.

Fig. 4 shows a scanning tube S', which is adapted to be used in cases where the image is projected from a position in front of the target and a scanning beam is applied from a position behind the target. 'Referring more particularly to Fig. 5, which is an enlarged perspective View of the assembly within the tube S', this tube comprises an evacuated container in which is mounted a composite target 5B, comprising a transparent supporting plate 5I of glass or similar material coated with a transparent metal layer 52 of a suitable substance such as silver, films 44 and 45, and a transparent conducting layer 45.- The lms and the conducting layer are similar to those described above with reference to Fig. 3. The external circuit is connected between the transparent metal layer 52 and the conducting layer 46 by a connection not shown in the drawings. 'I'he scanning beam is pro'duced by the fluorescent screen of the cathode ray tube C, this and the optical systems I9 and v2| being also similar to those disclosed in connection with Fig. 1. Image controlled radiations are projected through the transparent conducting layer 4B onto the photo-conducting nlm 45 to control its conductivity in accordance with the tone values of the object. The scanning beam B from the uorescent screen of the cathode ray tube C passes through the transparent plate 5I and the transparent conducting layer 52 to scan successively the elemental areas of the photo-conducting iilm 44 to impart conductivity to these elemental areas in succession. An image current is, therefore, produced which ows through the external circuit in a manner similar to that described above. 'I'his arrangement will also operate in accordance with the storage method described above.

Figs. 6, 7 and-8 each includes a target, similar to that disclosed with reference to Fig. 5 except for the differences noted below in the description of each gure, mounted on the external surface glflbihce end wall GII of the scanning cathode ray In Fig. 6, the end wall 60 takes the place of 1e glass plate 5| of Fig. 5, but the target is otherise similar. It comprises a transparent metal .yer 52, preferably of silver, two photo-conductlg films 44 and 45 of diierent materials, respecvely similar to the photo-conducting iilms de- :ribed in connection with Fig. 3, and a conductlg layer 46 of silver or the like. While the glass iclosure 6| for the target is shown attached to ie end wall of the cathode ray tube C, it may be iaced therefrom and have the target mounted L a position intermediate the walls of the coniiner 6I. This construction would include a `ass plate similar to of Fig. 5. The operation the device shown in this figure is similar to that ascribed above with reference to Fig. 4.

In Fig. 7, the two photo-conducting lms are :ade of the same material and are separated by medium to prevent radiations applied to one lm from affecting the other film. The target.

ius comprises a transparent metallic layer 52, noto-conducting films 54 and 55, a thin, black, igh resistance layer 56, made of bakelite or simar material, placed between the two photo-conucting lms to prevent radiations applied to the lm 55 from affecting lm 54, and vice versa, and conducting layer 46. With this construction, 1e same type of radiations may be used to both luminate the image field and to scan the target. he method (or methods) of operation is similar i that of Fig. 6. The resistance layer 56 is so 1in and of such high specic resistance that its Iteral conductivity is small with respect to its 'ansverse conductivity.

Fig. 8 shows a target in which a singlellm 62 mounted between the conducting layers 52 and i and is just thick enough to prevent both the :anning beam and the radiations applied to the nage eld from aiecting it throughout. This rrangement permits the use of the same type idiations for both illuminating the field and :anning the target. The lm 62, as well as the lms 54 and 55 of Fig. 7, may be made of the samelaterial as either lm 44 or 45 of Fig. 3, dependlg on the type of radiations it is desired to use. he operation of the device shown in this iigure similar to that described above in connection ith Fig. 7, the single thick'film 62 of this figure erforming the functions of both lms 54 and 55 E Fig. 7. In this gure, as well as in Fig. 7, 1e glass enclosure 6I has been omitted but it preferable to have such an enclosure to pro- :ct the thin layers or lms comprising the target. In Figs. 6 to 8, inclusive, an optical system I9, milar to that shown in Fig. 1, may be used for rojecting radiations from the image O on the irget. It would also be satisfactory to use the me type of external circuit as used in that iig- While this invention has been shown as applied r the situation where the object is a human beig, it will be apparent that the invention is also pplicable to the transmission of outdoor scenes motion picture films, either using radiations :flected from the film, or passing through it, to ntrol the operation of the scanning screen or Lrget.

While several specific embodiments for utilizlg the invention have been disclosed, it is to e understood that this invention is not limited iereto, but only by the scope of the appended aims. In these claims, the term sensitive to idiations as used to describe certain elements intended to include both photo-conducting and hoto-emissive materials.

What is claimed is:

1. An electro-optical system comprising a thin plate-like photoelectric member appreciably s'ensitive only to radiations of a certain wave-length range, a second thin plate-like photoelectric member appreciably sensitive only to radiations of a different Wave-length range, said first memt ber being at least partially transparent to radiations Within said second range, said photoelectric members being contiguous to each other, means for impressing radiations of both said ranges said conductive element through said source of' potential to all portions of saidsecond'photoelectric member, whereby radiations of one of said ranges act on one only of said photoelectric members to condition the system and radiations of the other of said ranges act on the other only of said photoelectric members to cause the formation of a signal current in said impedance element.

2. An electro-optical system comprising a thin plate-like photoelectric member appreciably sensitive only to radiations of a certain wave-length range, a second thin plate-like photoelectric member appreciably sensitive only to radiations of a diierent wave-length range, said rst member being at least partially transparent to radiations within said second range, said photoelectric members being contiguous to each other and at least one of said members being photoconducting, means for impressing radiations of both said ranges simultaneously on both said members from the side on which said first member is located, said means comprising means for projecting an imageof an object eld on said members with radiations of one of said ranges, and means for scanning said members element by element with radiations of -the other of said ranges, a conductive element adjacent the first photoelectric member, a source of potential, and means including an impedance element for completing a circuit from said conductive element through said of said ranges act on one only of said photoelec-l tric members to condition the system and radiations of the other of said ranges act on the other only of said photoelectric members to cause the formation of a signal current in said impedance element.

3. In combination, a thin plate-like photoemissive member appreciably sensitive only to radiations of a certain wave-length range, a thin plate-like photoconducting member contiguous to said photo-emissive member and appreciably sensitive only to radiations of a different wavelength range, said photo-emissive member being at least partially transparent to radiations within said second range, means for limpressing radiations of both said ranges simultaneouslyx on both of said members from theside on which said photo-emissive member is located, said means comprising means for projecting an image of an object eld on said members with radiations of one (if said ranges, and means for scanning said members element by element with radiations of theother of said ranges, a conductive element spaced from said photo-emissive member, a source of potential, and means for completing a circuit from .said conductive element through said source of potential to all of the elements of said photoconducting member, whereby radiations of one of said ranges causes the emission of I electrons from said photo-emissive layer to said conductive element and radiations of the other of said ranges changes the conductivity of each element of said photoconducting member in accordance `with the intensity of said radiations on said elements.

4. An electro-optical system comprising a first thin plate-like photoconducting member appreciably sensitive only to radiations 'of a certain wavelength range, a second thin plate-like photoconducting member contiguous to said rst photoconducting member and apprecably sensitive only to radiations of a different wave-length range, said-rst member being at least partially transparent to radiations within said second range, means for impressing radiations of both said ranges simultaneously on both said members from the side on which said first member is located, said means comprising means for projecting an image of an object eld on said members with radiations of one of said ranges, and means for scanning said members element by element with radiations of the other of said ranges, a con- I ductive element adjacent the rst photoconducting member, a source of potential, and means including an impedance element for completing a circuit from said conductive element through said source of potential to all the elements of said second photoconducting member, whereby radiations Vof one of said ranges changes the conductivity of all the elemental areas of one of said photoconducting members and radiations of the other of said ranges makes various elements of the second photoconducting member appreciabiy conducting in turn so that a signal current passes through said impedance element.

' FRANK GRAY. 

